Loading in 5 sec....

Force Analysis of MachineryPowerPoint Presentation

Force Analysis of Machinery

- 44 Views
- Uploaded on
- Presentation posted in: General

Force Analysis of Machinery

Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author.While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server.

- - - - - - - - - - - - - - - - - - - - - - - - - - E N D - - - - - - - - - - - - - - - - - - - - - - - - - -

- Introduction:
In a dynamic analysis, we create equations that relate force and motion of a body (as in ME 233) or in our case a mechanism or machine. These are called equations of motion.

There are 2 directions to these problems: the Forward Dynamics problem, where the motion is given and the forces are to be determined, and the Inverse Dynamics problem, where the driving force is given and the resulting motion is to be found.

Forward kinematics: We will call our method Kinetostatics – look for dynamic equilibrium at a specific position and time, a snapshot of the mechanism.

The equations will look like:

With m, a known, F unknown, or for a mechanism:

The eq’s for force are linear and solved using linear algebra

Inverse dynamics: Called the time-response problem. This solves the motion of a mechanism given the input driving force. Force example, the time history of the flight of an arrow leaving a bow.

For these problems, we write equations of motion (which are now differential eqations of motion) that might look like:

And solve motion as a function of time through numerical integration. For ex.

Forward Dynamics:

“Kinetostatics”

Given motion, find required driving force and all bearing reactions

- Inverse Dynamics:
- “Time response”
- Given input force, solve output motion as a function of time.

- Performing force analysis of a mechanism draws on all your modeling skills:
- Mechanism modeling, position, velocity and acceleration analysis, force analysis

- Goals from this section:
- Learn how to carry out a force analysis (kinetostatics)
- Apply to several examples in class and HW.
- Create a computer model (Matlab) for force analysis and apply to a specific problem

- Newtonian mechanics:
- Conservation of momentum
- Force = rate of change of momentum
- Action/reaction

- Corollary, Euler’s Equation:
- Torque = rate of change of angular momentum

- Dynamic forces:
- Linear acceleration:
Acceleration of pt. P:

Sum forces on particle P:

And integrate to solve:

Result: **

- Linear acceleration:

- Dynamic Moments:
- General layout shown in figure:

- Dynamic Moments (cont.):
- Sum moments about point D for particle P, then integrate over the body:
- Results: I is about c.g.
- If summed about c.g. (point g)

- 2-force member:
A link is a 2FM if it satisfies 3 conditions:

- It has revolutes at each end
- No loads other than at the endpoints
- Mass is negligible compared to the load
All forces lie along direction of the link

- Superposition:
- Given a mechanism with known position, velocity, and acceleration conditions, derive Newtons equations for dynamic equilibrium. These equations are linear in the forces and therefore Superposition principles can be applied: Inertial and applied forces on each link can be considered individually and then superposed to determine their combined effect.
- This approach is good for building intuition and solving by hand.
- This approach can be very long

- Matrix Method
- All inertial and applied forces are considered at once. The dynamic equations become coupled in the unknown forces and are solved using linear algebra techniques.
- Note: Why are forces linear?
- This approach is the best for computer application, therefore our method of choice.

- Energy method (Virtual work):
- Here, only forces that do work on the mechanism are considered. An equation of conservation of energy is written that results in 1 scalar equation with 1 unknown (for a 1 dof system)
- This is the easiest method if only the input force is required.

- To find driving and bearing forces using superposition, break the problem into n-1 parts. For ex.
- Find Tin’ = due to forces on link n
- Find Tin’’ = due to forces on link n-1
- Find Tin’’’’’’ = due to forces on link 2

- Notes:
- Notation: F14 = force of link 1 on link 4
- Be careful with signs
- F14=-F41,
- But, remember to either switch the sign, or the direction of the vector, but not both
- T=rxF

- Break the problem into n-1 parts, n = number of links.
- Start with part 1
- Draw FBD’s of the extreme link
- Include all forces for Part 1 ONLY
- Look for 2FM’s to reduce unknowns
- Solve unknown reaction forces as 3 eq’s, 3 uk’s (in general)
- 3 equations are:

- Move to the next link, transferring forces from the previous as,
- F23=-F32 (or, changing the directions on the vectors and keeping the magnitude)

- Continue to the driving link, solve for Tin’

- Repeat, solving Tin’’

- Tin(tot) = Tin’+Tin’’+Tin’’’+ …
- F12x(tot)= F12x’+ F12x’’+…
- Etc.

Given:

- P=10,45deg, R=10i, T4=5k
- m2=0,m3=1,m4=sqrt2
- I2=0, I3=1, I4=1
- ag3=-1i+1j, ag4=-1j
- a3=0, a4=1
Find: Tin and reactions at grd. bearings

- Hydraulic-powered scoop with a load in bucket (link 4)

- Links 2 & 4 have mass
- m2 = 10 kg, I2 = 1 kgm^2
- m4 = 100 kg I4 = 10 kgm^2

- Consider the cylinder, 5 as a 2 FM. Given the following motion information, find the input cylinder force and the bearing reactions at points O2 and O5.
- Motion info:
- w2=1, a2=1 rad/s^2w4=1, a4=1 rad/s^2
- Vg2=-1i+0j m/sVg4=-1i+1j m/s
- Ag2=01i-1j m/s^2Ag4=-2i+0j m/s^2
- Vp=2j

- Force on bucket:
- P = 100N

In the matrix method, equations of dynamic equilibrium are written for FBD’s of all the links in the mechanism w/ all internal and external forces included. This results in a coupling of the unknown forces. However, the equations are linear in these forces and may be solved using linear algebra techniques.

For example:

Solving forces:

Known motion info

Known coefficients

Unknown forces and torques

In a general mechanism, there may be anywhere from 10 to 30 unknown forces to solve. Solve in Matlab (or other computer program)

This method will be demonstrated first on a four-bar linkage.

The figure above shows a general 4-bar linkage. The center of mass of each link is shown, as well as the input torque on link 2, and an applied torque (T4) on link 4.

Here, we have included some additional vectors to help define our problem. This leads to the following notation:

gi = center of mass of link i

jti = joint i

rij = vector from cm of i to jt. j

Fij = vector force of i on j

- Count the number of unknowns:
- There are two unknown forces at every 1 dof joint
- There is one unknown force for every input

- Count the number of equations:
- There are three equations for each body

- In this example:
- # unknowns = 9
- # equations = 9

Solve for the input torque and all bearing reactions using the matrix method – set up the linear system of equations in matrix form.

- Links 2 & 4 have mass
- m2 = 10 kg, I2 = 1 kgm^2
- m4 = 100 kg I4 = 10 kgm^2

- Consider the cylinder, 5 as a 2 FM. Given the following motion information, find the input cylinder force and the bearing reactions at points O2 and O5.
- Motion info:
- w2=1, a2=1 rad/s^2w4=1, a4=1 rad/s^2
- Vg2=-1i+0j m/sVg4=-1i+1j m/s
- Ag2=01i-1j m/s^2Ag4=-2i+0j m/s^2
- Vp=2j

- Force on bucket:
- P = 100N

- Multiple links @ 1 joint
At this joint, there are 2 unknown vector reactions, say F12 and F13

- Gears:
The direction of the force between the gears is known (along the common normal), with the magnitude unknown

- Hydraulic Cylinder:
- Model as 2 rigid bodies, to result in an a fluid pressure force, a normal-wall force, and a wall torque
- Model as a two force member, then there is one unknown, the force in the member (* preferred)

- If a rigid body is in equilibrium under the action of external forces, the total work done by these forces is zero for a small displacement of the body.
- Work:
- With F, x, T, q, vectors and W a scalar.
- To indicate that we are dealing with infinitesimal displacements (virtual displacements), use the notation:

- Now apply the virtual work definition:

- If we divide the virtual work by a small time step, we get:
- These are all external torques and forces on the body, and include inertial forces and gravity. Rewrite, to clearly show this as:
With:

- Notes
- Solve the driving force of a single dof system with a single scalar equation
- Internal forces (ex. Bearing reactions) cannot be solved with this technique.

- Links 2 & 4 have mass
- m2 = 10 kg, I2 = 1 kgm^2
- m4 = 100 kg I4 = 10 kgm^2

- Consider the cylinder, 5 as a 2 FM. Given the following motion information, find the input cylinder force and the bearing reactions at points O2 and O5.
- Motion info:
- w2=1, a2=1 rad/s^2, w4=1, a4=1 rad/s^2
- Vg2=-1i+0j m/sVg4=-1i+1j m/s
- Ag2=-1i-1j m/s^2Ag4=-2i+0j m/s^2
- Vp=2j, V5=1i+1j

- Force on bucket:
- P = 100N